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Filip Meysman, Stijn Bruers, Jack Middelburg

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From Carnot engines to dissipative structures ... Ascendency (Ulanowicz, 1986) Exergy. Eurandom 2005. Slide 06/38. ASLO 2005 Santiago. Slide 02/15 ... – PowerPoint PPT presentation

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Title: Filip Meysman, Stijn Bruers, Jack Middelburg


1
Thermodynamics and Ecology from Carnot engines
to ecosystems
Filip Meysman, Stijn Bruers, Jack Middelburg
Netherlands Institute of Ecology
(NIOO-KNAW) Centrum Estuarine en Marine
Ecology Department Ecosystem Studies Korringaweg
7, 4401 NT Yerseke
Slide 01/15
2
Outline of the presentation
  • Thermodynamics and ecology Two fields in a state
    of confusion? (personal view)
  • From Carnot engines to dissipative structures
  • Many dissipative structures boycotting each
    other turbulence and ecosystems (intro to
    Stijns work)

Eurandom 2005
Slide 02/38
3
Part 1 Thermodynamics and Ecology two fields
in a state of confusion?
Slide 01/15
4
Thermodynamics and ecology?
Theory
  • Ecosystems are macroscopic physical systems
  • Thermodynamics is that part of the physics theory
    that deals with macroscopic phenomena (not too
    small -gt quantum, not too big -gt relativity)
  • Conclusion thermodynamic principles should in
    theory be applicable to ecology

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 04/38
5
Ecologists liberal use of thermodynamics
  • Fuzzy terminology using terms without proper
    definitions (e.g. organisms are dissipative
    structures)
  • Using concepts out of context

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 05/38
6
Ecologists do not like entropy
A range of other y-ending properties are defined
to characterize the functioning of an ecosystem
  • Emergy (Odum,1983)
  • Ascendency (Ulanowicz, 1986)
  • Exergy
  • .

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 06/38
7
Are ecologists the only one to blame?
Thermodynamics comes in many different flavours
  • Equilibrium thermodynamics (Carnot, Clausius,
    Gibbs)
  • Linear non-equilibrium thermodynamics (Onsager)
  • Rational thermodynamics (Truesdell)
  • Far-from-equilibrium thermodynamics (Prigogine)
  • Extended thermodynamics
  • Finite-time thermodynamics

These different theories are not necessarily
inter-consistent, nor is the link clear between
them.
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 07/38
8
Speaking in many tongues
The Second Law
  • 29 different formulations of the Second Law
  • Bluff you way into the Second Law of
    Thermodynamics (Uffink, 2001)
  • Essential conflict between the Kelvin-Planck
    formulation and that of Caratheodory (1909)
    remains unsolved
  • There is more than just terminological confusion

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 08/38
9
Present theory is subjective ?
The First Law
(Energy change Heat work)
environment
Adiabatic expansion
system
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 09/38
10
Link between thermodynamics and ecology
Summary
  • Thermodynamic modeling theory itself is not fully
    mature and crystallized
  • Sloppy application of thermodynamics in ecology
    (based on intuition, with little quality
    control)

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 10/38
11
Part 2 From Carnot engines to dissipative
structures
Slide 01/15
12
Carnot engine
High-temperature reservoir
1 Thermal conduction over Infinitely small
temperature gradients 2 No frictional losses
QH
Working fluid cycle
Pump
QL
Low-temperature reservoir
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 12/38
13
Analysis Carnot engine
Work produced in one cycle
Heat discarded in low-temp-res
Entropy production per cycle
Power output
Entropy production
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 13/38
14
Steam engine
Two types of entropy production 1 Thermal
conduction over finite temperature gradients 2
Frictional losses momentum Transfer over
velocity gradient
QH
Boiler
Working fluid
Condenser
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 14/38
15
Steam engine steady-state analysis
Work produced in one cycle
Heat discarded in low-temp-res
Entropy production per cycle
Power output
Entropy production
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 15/38
16
Freak engine
QH
Boiler
All the work produced is delivered back to the
engine to increase the cycling frequency
Working fluid cycle
Condenser
QH
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 16/38
17
Steady-state analysis Freak engine
Work produced in one cycle
Heat discarded in low-temp-res
Entropy production per cycle
Power output
Entropy production
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 17/38
18
Two modes of operation
Freak engine does cycle -gt
Freak engine does not cycle
Positive feedback
Th
Th
Kinetic energy
Friction
Tl
Tl
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 18/38
19
Freak engine Entropy production
Cycling mode stable branch
Total entropy production
No-cycling mode stable branch
Critical threshold
Driving force
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 19/38
20
Freak engine dissipative structure
Atmospheric fluid dynamics
QH
Working fluid cycle
Organisms Ecosystems
QH
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 20/38
21
Hurricane upside down Freak engine
Warm sea water
Positive feedback
Warm air
Kinetic energy
Turbulence
Cold air
Cold stratosphere
Driving force
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 22/38
22
Benard-Rayleigh cell Entropy production
Total entropy production
Thermal convection stable branch
Thermal conduction stable branch
Critical threshold
Driving force
Nature abhors a gradient Schneider Sagan
(2005)
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 22/38
23
Bacteria freak engine
Glucose reservoir
Positive feedback
Glucose
Bacterial growth in chemostat
Bacterial biomass
Cell Turn-over
CO2
CO2 reservoir
Driving force
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 23/38
24
Bacterial growth in chemostat
1. Respiration
CO2
Gluc
Glucose reservoir
ATP
ADP
Positive feedback
Glucose
2. Biomass synthesis (work)
Bacterial biomass
Gluc
Biomass
Cell Turn-over
CO2
ADP
ATP
3. Biomass turn-over (friction)
Waste reservoir
Biomass
Gluc
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 24/38
25
Bacterial growth in chemostat
Mass balance reactor glucose (Ch)
Exchange with reservoirs
Glucose consumption
Recycling Biomass turn-over
Mass balance reactor CO2 (Cl)
Exchange with reservoirs
Respiration
Mass balance bacterial biomass (B)
Biomass turn-over
Growth
See presentation Stijn Bruers
Eurandom 2005
Slide 25/38
ASLO 2005 Santiago
Slide 02/15
26
Two modes of operation
Biological oxidation
Chemical oxidation
Positive feedback
Ch
Ch
Bacterial biomass
Turn-over
Cl
Cl
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 26/38
27
Entropy production in chemostat
Overall conversion
Total entropy production
Bacterial oxidation stable branch
This graph only shows the effect of one organism
feeding on an abiotic food source!
Pure chemical oxidation stable branch
Critical threshold
Driving force
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 27/38
28
Part 3 Many dissipative structures boycotting
each other
Slide 01/15
29
Turbulent cascade
Warm air
Large Eddy
Smaller Eddy
Smaller Eddy
Smaller Eddy
Cold air
  • Smaller eddies feeding on larger eddies, on to
    viscous dissipation

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 29/38
30
Energy transport from tropics to polar regions
Emission terrestrial radiation
Incoming solar radiation
Poles
Tropics
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 30/38
31
Simplified equation set
Linearization of Wiens Radiation Law leads to
(Kleidon and Lorenz, 2005)
Temperature tropics
Tropic temperature
Pole temperature
Temperature pole
Eurandom 2005
Slide 31/38
ASLO 2005 Santiago
Slide 01/15
32
Energy transport from tropics to polar regions
Emission terrestrial radiation
Incoming solar radiation
Poles
Tropics
Net energy transfer
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 32/38
33
Maximum entropy production
Temperature tropics
Tropic temperature
Complete universe
Pole temperature
Atmospheric circulation
Temperature pole
Eurandom 2005
Slide 33/38
ASLO 2005 Santiago
Slide 01/15
34
Maximal entropy production
To good to be true?
  • MEP value of heat transport coefficient k 2 W
    m-2 K-1
  • MEP state conforms with observations on the Earth
    climate system equator-pole temperature profile,
    intensity of athmospheric circulation, cloud
    cover (Paltridge 1975)
  • Confirmed by general circulations model
    simulations (Shimokawa and Ozawa, 2001)
  • MEP on other planets Mars and Saturns moon
    Titan

ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 34/38
35
Food chain in food web marine sediments
Organic matter from water column
Bacteria
Ciliates
Copepods
Predator polychaet
CO2
  • Larger predators feeding on smaller prey

ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 35/38
36
Food web in a marine sedimens
Input from water column
Accumulation deeper sediments
Accumulation deeper sediments
Food web
Organic matter from water column
CO2
Net conversion
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 36/38
37
Entropy production.
Equations for a chemostat ecosystem are
completely analogous
Complete universe
Food web conversion
Eurandom 2005
Slide 37/38
ASLO 2005 Santiago
Slide 01/15
38
Conclusions
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 38/38
39
Steam engine Dynamic operation
Energy
Kinetic energy
Internal energy condenser
Internal energy boiler
High temp reservoir
Kinetic energy
Low temp reservoir
ASLO 2005 Santiago
Slide 01/15
Eurandom 2005
Slide 02/38
40
Freak steam engine dissipative structure
Energy balance warm air currents
Warm Seawater
Q
Conversion
Transfer from sea water
Positive feedback
Energy balance cold air currents
Kinetic energy
Transfer from warm air
Transfer to stratosphere
Frictional loss
Q
Kinetic energy balance
Cold stratosphere
Frictional force
Driving force
ASLO 2005 Santiago
Slide 02/15
Eurandom 2005
Slide 02/38
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